WO2013101379A1 - Appareil de collecte de signaux de cathodoluminescence - Google Patents
Appareil de collecte de signaux de cathodoluminescence Download PDFInfo
- Publication number
- WO2013101379A1 WO2013101379A1 PCT/US2012/066770 US2012066770W WO2013101379A1 WO 2013101379 A1 WO2013101379 A1 WO 2013101379A1 US 2012066770 W US2012066770 W US 2012066770W WO 2013101379 A1 WO2013101379 A1 WO 2013101379A1
- Authority
- WO
- WIPO (PCT)
- Prior art keywords
- sample
- fiber optic
- ellipsoid
- collection
- light
- Prior art date
Links
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J37/00—Discharge tubes with provision for introducing objects or material to be exposed to the discharge, e.g. for the purpose of examination or processing thereof
- H01J37/02—Details
- H01J37/22—Optical or photographic arrangements associated with the tube
- H01J37/226—Optical arrangements for illuminating the object; optical arrangements for collecting light from the object
- H01J37/228—Optical arrangements for illuminating the object; optical arrangements for collecting light from the object whereby illumination and light collection take place in the same area of the discharge
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J37/00—Discharge tubes with provision for introducing objects or material to be exposed to the discharge, e.g. for the purpose of examination or processing thereof
- H01J37/26—Electron or ion microscopes; Electron or ion diffraction tubes
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J2237/00—Discharge tubes exposing object to beam, e.g. for analysis treatment, etching, imaging
- H01J2237/20—Positioning, supporting, modifying or maintaining the physical state of objects being observed or treated
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J2237/00—Discharge tubes exposing object to beam, e.g. for analysis treatment, etching, imaging
- H01J2237/244—Detection characterized by the detecting means
- H01J2237/2445—Photon detectors for X-rays, light, e.g. photomultipliers
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J2237/00—Discharge tubes exposing object to beam, e.g. for analysis treatment, etching, imaging
- H01J2237/244—Detection characterized by the detecting means
- H01J2237/24495—Signal processing, e.g. mixing of two or more signals
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J2237/00—Discharge tubes exposing object to beam, e.g. for analysis treatment, etching, imaging
- H01J2237/26—Electron or ion microscopes
- H01J2237/28—Scanning microscopes
- H01J2237/2803—Scanning microscopes characterised by the imaging method
- H01J2237/2808—Cathodoluminescence
Definitions
- This invention relates to the field of electron microscopy and in particular to the collection cathodoluminescence signals.
- CL Cathodoluminescence
- TEM has been achieved using off-axis parabolic mirrors which provide direct optical coupling through a side vacuum window.
- the specimen is held at the focal point of these mirrors, light is then collimated and can be coupled to other transmission or detection apparatuses.
- this approach is restricted to TEM microscopes with a wide pole piece gap (e.g. >6mm) and with an appropriate additional port to position the mirror above the specimen.
- Cathodoluminescence can be weak in a TEM because the volume stimulated by the electron beam is small. This is because the specimen is normally thin enough to be partially transparent to electrons at the desired working accelerating voltage.
- Cathodoluminescence is normally analyzed in terms of size of signal (panchromatic imaging), size of a specific bandpass, (monochromatic or filtered imaging), and spectroscopic mapping. It can also be analyzed as a function of time, from picoseconds resolution to evolution over some hours. The efficiency of cathodoluminescence varies very significantly depending on specimen type, temperature, thickness and injection conditions. Efficient light collection is useful and sometimes essential to perform an experiment, especially if the signal must be measured simultaneously with other analytical measurements.
- TEM pole pieces and side entry holders provide hard restrictions on the available space to employ collection and transmission optics.
- a side entry Transmission Electron Microscope (TEM) holder holds a specimen on a goniometer in a tightly restricted volume. The restriction is given by the need to insert through the vacuum seal of the goniometer and by the pole piece gap of the TEM. In practice this means that almost all known TEM-CL solutions utilizing some form of collection optics are restricted to wide pole piece gap instruments (upper or lower gaps >4mm). The use of a wide pole piece gaps compromises the performance of the TEM when used for other analytical techniques. It is estimated that greater than 80% of TEMs installed worldwide are unsuitable for known TEM-CL technology due to the narrow pole pieces they employ. Thus an need exists for a solution that overcomes the space restrictions when employing collection optics.
- an apparatus for collection of cathodoluminescence from a sample under irradiation by electrons in an electron microscope includes sample carrier for a sample having a sample plane; a light collection mirror; a fiber optic transmission cable having a face.
- the light collection mirror is a reflective ellipsoid
- the ellipsoid surface situated to collect light from the sample.
- the ellipsoid has a first focal point at the sample and a second focal point as the fiber optic cable face.
- ellipsoid has an axis between the focal points, with the axis being tilted with respect to the sample plane.
- the face of said fiber optic transmission cable is tilted to optimize collection efficiency.
- the fiber optic transmission cable is a single silica core high numerical aperture fiber.
- the fiber optic transmission cable has a
- the fiber optic transmission cable has a core size of approximately .4 mm.
- the fiber optic transmission cable is stripped to
- the ellipsoid mirror is made of rapidly solidified
- the ellipsoid is tilted at an angle of approximately
- the sample is irradiated by ions instead of electrons.
- Fig. 1 is a cross sectional drawing of an exemplary device for efficient collection of cathodoluminescence signals
- Fig. la is an enlarged view of the device of Fig. 1.
- Fig. 2 is a cross sectional drawing of an exemplary tilted ellipsoid for use in the device of Fig. 1 ;
- Fig. 3 is a cross sectional drawing showing tilted ellipsoid mirrors, tilted fiber optic cables and a specimen.
- collection mirrors 10, 20 attached to the end piece of a side entry holder 1 collect light from the region of the sample at the intersection of the holder center line 80 and the opening centerline 70 and transmit it to a suitable detection system external to the TEM via fiber optic cables 40, 50.
- the fiber optic cables have faces 41, 51 tilted for maximum collection of light.
- a fiber optic is a useful conduit for light in places of tight constraint, but also where thermal conductivity is important to control.
- TEM holders very small variations in temperature can cause drift which is seen in high magnification images.
- fiber optics can be introduced into a holder operating at LN2 temperatures without the fiber causing thermal artifacts.
- fiber optics do not impact the thermal stability of a holder. This therefore allows imaging and analysis at high magnification with the specimen held at cryogenic temperatures.(Room temperature or high temperature versions of the holder are also possible).
- the light collection and transmission optics are built into the side entry holder the whole system is compact and the analytical equipment used to analyze the light can be a considerable distance away from the TEM column, e.g. in a neighboring room or building.
- the specimen can be considered to provide a plane of symmetry. In some TEMs, there is some asymmetry in the space above and below the holder. If the light output above and below the specimen were equal, then the collection efficiency can be doubled with a symmetrical design that collects light from above and below. In cases with unequal light output above and below the specimen, collection efficiency is still increased.
- the material for the reflective elliptical mirror must be of a non-magnetic conductive metal which can be manufactured to a precise mathematical shape. This is required to correctly reflect and focus light emitted from a region of interest on the specimen into the tilted fiber.
- rapidly solidified aluminum is used for the mirrors because this material enables precision machining of miniature light collection optics.
- silica core fiber with a core of 0.4mm is used with a multi mode NA of 0.37.
- a fiber of NA 0.22 is most commonly used in spectroscopy apparatus and this would be very inefficient by comparison.
- the silica core provides good spectral response over the range of wavelengths required for CL measurements.
- the inventors have manufactured and tested a design having a gap above the specimen of 2.25mm and below the specimen of 2mm.
- this design similar opposing off-axis elliptical mirrors and tilted fibers collect light from above and below the specimen simultaneously.
- the smaller gap below restricts the volume and hence solid angle captured by this mirror, but there remains symmetry in the focusing optics.
- the fibers are stripped to achieve the required bend radii at a compound bend close proximity cross over point as shown in Fig. 1.
- This invention provides access to the specimen with a removable mirror.
- the access can be designed to be on the other side of the specimen boat to the mirror.
- the mirror may be removed and re-installed with a high degree of reproducibility as the mirror component locates on the TEM holder
Landscapes
- Chemical & Material Sciences (AREA)
- Analytical Chemistry (AREA)
- Investigating, Analyzing Materials By Fluorescence Or Luminescence (AREA)
Abstract
Priority Applications (4)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
EP12813163.8A EP2786395A1 (fr) | 2011-12-01 | 2012-11-28 | Appareil de collecte de signaux de cathodoluminescence |
JP2014544834A JP2015503198A (ja) | 2011-12-01 | 2012-11-28 | カソードルミネッセンス信号を収集するための装置 |
CN201280057308.9A CN103999185A (zh) | 2011-12-01 | 2012-11-28 | 阴极发光信号采集装置 |
AU2012363007A AU2012363007A1 (en) | 2011-12-01 | 2012-11-28 | Apparatus for collection of cathodoluminescence signals |
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
US13/309,026 | 2011-12-01 | ||
US13/309,026 US20130141803A1 (en) | 2011-12-01 | 2011-12-01 | Apparatus for collection of cathodoluminescence signals |
Publications (1)
Publication Number | Publication Date |
---|---|
WO2013101379A1 true WO2013101379A1 (fr) | 2013-07-04 |
Family
ID=47522895
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
PCT/US2012/066770 WO2013101379A1 (fr) | 2011-12-01 | 2012-11-28 | Appareil de collecte de signaux de cathodoluminescence |
Country Status (6)
Country | Link |
---|---|
US (1) | US20130141803A1 (fr) |
EP (1) | EP2786395A1 (fr) |
JP (1) | JP2015503198A (fr) |
CN (1) | CN103999185A (fr) |
AU (1) | AU2012363007A1 (fr) |
WO (1) | WO2013101379A1 (fr) |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
WO2016037198A1 (fr) * | 2014-09-12 | 2016-03-17 | Technische Universität Wien | Dispositif et système de transfert et de mesure de lumière produite par cathodoluminescence dans un microscope électronique à transmission |
EP2908328A4 (fr) * | 2012-10-04 | 2016-06-15 | Univ Seoul Nat R & Db Found | Dispositif de support pour microscope électronique |
Families Citing this family (6)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN106981411B (zh) * | 2017-05-03 | 2018-02-13 | 中国地质大学(北京) | 一种聚光系统及其聚光方法 |
JP7141874B2 (ja) * | 2017-09-29 | 2022-09-26 | 株式会社堀場製作所 | ルミネッセンス採光装置 |
EP3462475A3 (fr) | 2017-09-29 | 2019-11-20 | Horiba, Ltd. | Dispositif collecteur de luminescence |
CN111261478B (zh) * | 2018-11-30 | 2021-10-26 | 浙江大学 | 具有光纤的多自由度样品杆 |
EP3823004A3 (fr) * | 2019-10-23 | 2021-07-07 | Gatan Inc. | Système et procédé pour l'alignement d'optique à cathodoluminescence |
EP4133516A1 (fr) | 2020-04-07 | 2023-02-15 | Gatan, Inc. | Appareil de cathodoluminescence de microscopie électronique à transmission |
Citations (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
FR2617985A1 (fr) * | 1987-07-10 | 1989-01-13 | Centre Nat Rech Scient | Dispositif optique de collection de lumiere formant objectif a miroir de grande ouverture numerique |
JP2002162350A (ja) * | 2000-11-22 | 2002-06-07 | Hitachi Ltd | 蛍光測定装置 |
US20080181567A1 (en) * | 2007-01-31 | 2008-07-31 | Dana Craig Bookbinder | High numerical aperture fiber |
WO2011030156A2 (fr) * | 2009-09-10 | 2011-03-17 | University Of Sheffield | Collecte de rayonnement électromagnétique émis par des échantillons irradiés par des particules |
Family Cites Families (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US6885445B2 (en) * | 1998-05-09 | 2005-04-26 | Renishaw Plc | Electron microscope and spectroscopy system |
US20060060189A1 (en) * | 2004-08-30 | 2006-03-23 | Liu Yong Y | Optical reflector and optical collection system |
US7589322B2 (en) * | 2005-06-29 | 2009-09-15 | Horiba, Ltd. | Sample measuring device |
US8025445B2 (en) * | 2009-05-29 | 2011-09-27 | Baker Hughes Incorporated | Method of deployment for real time casing imaging |
-
2011
- 2011-12-01 US US13/309,026 patent/US20130141803A1/en not_active Abandoned
-
2012
- 2012-11-28 AU AU2012363007A patent/AU2012363007A1/en not_active Abandoned
- 2012-11-28 JP JP2014544834A patent/JP2015503198A/ja active Pending
- 2012-11-28 EP EP12813163.8A patent/EP2786395A1/fr not_active Withdrawn
- 2012-11-28 WO PCT/US2012/066770 patent/WO2013101379A1/fr unknown
- 2012-11-28 CN CN201280057308.9A patent/CN103999185A/zh active Pending
Patent Citations (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
FR2617985A1 (fr) * | 1987-07-10 | 1989-01-13 | Centre Nat Rech Scient | Dispositif optique de collection de lumiere formant objectif a miroir de grande ouverture numerique |
JP2002162350A (ja) * | 2000-11-22 | 2002-06-07 | Hitachi Ltd | 蛍光測定装置 |
US20080181567A1 (en) * | 2007-01-31 | 2008-07-31 | Dana Craig Bookbinder | High numerical aperture fiber |
WO2011030156A2 (fr) * | 2009-09-10 | 2011-03-17 | University Of Sheffield | Collecte de rayonnement électromagnétique émis par des échantillons irradiés par des particules |
Non-Patent Citations (1)
Title |
---|
CARLSSON L ET AL: "An efficient apparatus for studying cathodoluminescence in the scanning electron microscope", JOURNAL OF PHYSICS E. SCIENTIFIC INSTRUMENTS, IOP PUBLISHING, BRISTOL, GB, vol. 7, no. 2, 1 January 1974 (1974-01-01), pages 98 - 100, XP002409517, ISSN: 0022-3735, DOI: 10.1088/0022-3735/7/2/009 * |
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
EP2908328A4 (fr) * | 2012-10-04 | 2016-06-15 | Univ Seoul Nat R & Db Found | Dispositif de support pour microscope électronique |
US10312050B2 (en) | 2012-10-04 | 2019-06-04 | Snu R&Db Foundation | Holder device for electron microscope |
WO2016037198A1 (fr) * | 2014-09-12 | 2016-03-17 | Technische Universität Wien | Dispositif et système de transfert et de mesure de lumière produite par cathodoluminescence dans un microscope électronique à transmission |
Also Published As
Publication number | Publication date |
---|---|
CN103999185A (zh) | 2014-08-20 |
JP2015503198A (ja) | 2015-01-29 |
AU2012363007A1 (en) | 2014-06-26 |
EP2786395A1 (fr) | 2014-10-08 |
US20130141803A1 (en) | 2013-06-06 |
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